3D Simulations of Secondary Electron Generation in Diamond and RF Gun Modeling with VORPAL - PowerPoint PPT Presentation

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3D Simulations of Secondary Electron Generation in Diamond and RF Gun Modeling with VORPAL

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Title: 3D Simulations of Secondary Electron Generation in Diamond and RF Gun Modeling with VORPAL


1
3D Simulations of Secondary Electron Generation
in Diamond and RF Gun Modeling with VORPAL
Tech-X Corporation
D. A. Dimitrov
Main contributors D. Bruhwiler, R. Busby, D.
Smithe, P. Messmer, J. R. Cary, Ilan Ben-Zvi, T.
Rao, D. Kayran
Work supported by the US Dept. of Energy.
2
Collaborators
  • Ilan Ben-Zvi
  • T. Rao
  • D. Kayran
  • J. Smedley
  • X. Chang
  • Q. Wu
  • Brookhaven National Lab
  • D. L. Bruhwiler
  • R. Busby
  • D. Smithe
  • P. Messmer
  • C. Nieter
  • J. R. Cary
  • VORPAL developers
  • Tech-X Corporation
  • J. Lewellen
  • Argonne National Lab

5
3
Motivation-I
  • A new design for a photoinjector was recently
    proposed using diamond as an amplifier of primary
    electrons.
  • The design is very promising for generation of
    high-current, high-brightness electron beam.
  • Experiments have demonstrated the viability of
    the concept but the optimal design and parameters
    of operation are still being investigated.
  • Realistic PIC simulations of a photoinjector with
    a diamond amplifier are currently not available.
  • Such simulations are expected to provide valuable
    guidance when designing these devices.

4
Motivation-II
  • Generation of high order modes in an SRF electron
    gun with high average and peak current is a
    serious concern.
  • Only a fully electromagnetic code can study this
    problem.
  • The 3D massively parallel particle-in-cell (PIC)
    code VORPAL is uniquely suited for this
    application.
  • Investigate how VORPAL compares with PARMELA to
    model RF gun properties.

5
5
Schematic diagram of a secondary emission
enhanced photoinjector (SEEP) courtesy of
Triveni Rao
6
Physical Processes Involved
  • Elastic scattering - implemented two models
  • Isotropic and small angle scattering more
    accurate model currently considered
  • Inelastic scattering for secondary electron and
    hole generation that takes band structure into
    account - implemented
  • Electron-hole recombinations
  • Acoustic and optical phonon scattering
    (inelastic)
  • Scattering from impurities and defects
  • Emission from diamond surfaces taking into
    account different electron affinities.

5
7
Total Elastic and Inelastic Scattering Cross
Sections
  • mean free time
  • mean free path

8
Generation of Secondary Electrons and Holes
  • General Monte Carlo algorithm implemented for
    scattering processes
  • Electrons or holes with Ekin gt EG (5.46 eV) can
    generate secondaries

5
9
PDF for the Primary Electron Momentum Change
10
Energy Loss Function
11
Sampling from the PDF for the Primary Electron
Momentum Change
12
Yield of Secondary Electrons is in Fair Agreement
with Previous Simulations
EC 29 (eV) EG 5.46 (eV)
Ep 1000 EC (eV)
Ep 250 EC (eV)
  • Two limiting cases considered
  • With energy loss to lattice
  • No energy loss to lattice
  • Averages for Ne are over 200 runs.

13
Yield of Secondary Electrons is in Fair Agreement
with Previous Simulations
  • Comparison is not under the same conditions.
  • Bejata et al. reported

14
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16
VORPAL Geometry Representation Capability
  • VORPAL software is able to do curved surfaces
    modeling.
  • Improves accuracy of wakefield and HOM coupling
    and propagation through apertures.
  • Cavity focusing and defocusing effects during
    acceleration-deceleration passes.

17
VORPAL Provides Second Order Accuracy for 3-D
Accelerating Cavities
  • Most codes use stair-step (first order accurate)
    boundaries.

18
Geometry Representation for the 1.5 Cell RF Gun
Developed in BNL
  • 3D VORPAL representation.
  • SUPERFISH axially symmetric description.

19
Simulation Parameters
  • RF field frequency 703.75 MHz
  • RF field at cathode surface at t 0 -8.28 MV/m
  • RF phase 40 degrees
  • RF field amplitude 30 MV/m
  • Beer can beam shape with approximately 5 nC total
    charge
  • Beam radius 4 mm
  • Beam length 80 ps

Ez (MV/m)
z (cm)
  • Multi bunch simulations
  • Bunches emitted at each RF period
  • 3.5 A average current
  • Only at lowest grid resolution currently

20
VORPAL Average Kinetic Energy Agrees Well with
PARMELA
  • Provides confirmation that accelerating RF fields
    are approximately correct.

5
21
Wakefield effects cause less than 1 variation
in Ekin for multi bunch runs
5
22
Comparison of RMS Bunch Length - I
  • VORPAL results show shorter bunch length but
    getting close to the PARMELA result when
    increasing the longitudinal grid resolution.

5
23
Comparison of RMS Bunch Length - II
  • The behavior is qualitatively similar.

24
Multi Bunch Variation in Zrms
  • The wakefieds cause variation in the range
  • -1 lt Zrmslt 4
  • Most beams are shorter than the first beam by 1
  • The 8th beam is longer by 4 .

25
VORPAL Shows Qualitatively Similar Transverse RMS
Size Behavior
  • The observed transverse rms size was smaller in
    VORPAL (the beam was emitted with no thermal
    velocities).

5
26
Wakefield Effects on the Transverse RMS Size
  • Consecutive bunches expand transversely by 3
    relative to the first bunch.

5
27
RMS Emittance - I
  • Further studies are needed to understand the
    differences in the rms emittance, particularly
    the effect of wake fields included in VORPAL self
    consistently.

5
28
RMS Emittance - II
  • At the exit of the gun, VORPAL shows about 3
    times larger emittance. Detailed convergence
    simulation at different parameter sets should
    provide better understanding of the importance of
    different algorithms.

5
29
Multi Bunch Simulations Show Small Emittance
Increase
  • On average, the increase at the exit is 4 .
  • Emittance varies from -2 to 4 .

5
30
Summary and Future Work
  • 3D parallel PIC simulations with VORPAL
    demonstrated that the code is uniquely suited for
    SRF electron gun studies.
  • Initial simulations and benchmarking of VORPAL
    results show quantitative agreement with PARMELA
    for some beam parameters and qualitative for
    others.
  • Future studies will focus on
  • Completing algorithms for
  • electron-hole transport in diamond
  • emission of electrons from diamond surfaces
  • higher accuracy algorithms,
  • simulation studies with PML boundary conditions,
  • more accurate treatment of RF fields
  • investigation of higher order modes

5
31
Acknowledgments
This work was supported by the US Department of
Energy, office of Nuclear Physics, under an SBIR
grant and Tech-X Corp.
5
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